We use the density functional theory to invest&te the ground state cner,g of 5 psir of intemcting electronic syslcr;ls ;ct large distanCcs from one another. We prove that a simple mean field approximation to the electron density is sufficient to determine the6(1/R3) and(i(l/R$) behavior of the groun
Prospects for a van der Waals density functional
β Scribed by John F. Dobson
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 125 KB
- Volume
- 69
- Category
- Article
- ISSN
- 0020-7608
No coin nor oath required. For personal study only.
β¦ Synopsis
The van der Waals vdW or dispersion interaction between distant sections of a molecular or condensed matter system contributes part of the correlation energy. This dispersion part is missed, or is given at best unreliably, by the usual local and gradient functionals for the exchangeαcorrelation energy. Here we discuss various quasi-local schemes which are expected to provide good vdW energies using only a Ε½ . knowledge of the ground-state electron density n r . The general scheme proposed is ''seamless,'' i.e., it remains valid whether or not the subsystems involved have significant overlap of electronic density. Perturbative expansion of this scheme, followed by a doubly local density approximation, yields a simple vdW scheme proposed independently by Andersson et al. and by Dobson and Dinte, which is also similar to a scheme of Rapcewicz and Ashcroft. These simpler schemes cannot deal with overlap between the electron clouds. Progress is reported on the full seamless scheme which deals with the more challenging case where overlap is present. All of the present schemes yield the classic dipolar '' van der Waals'' 1rR 6 energy when the separation R sufficiently exceeds the individual system dimensions. None is restricted to this case, however.
π SIMILAR VOLUMES
On the basis of the adiabatic connection formula we propose several approximations for the total correlation energy functional, which, in the limit of two separated neutral subsystems, correctly reproduce the van der Waals R y6 behavior. We have calculated the corresponding van der Waals coefficient